H Y D
imrerr~t\ly,
as in the ehaleedoryy ; and giving a gene–
r.i1 clouuinefs or millinefs to thc 1I0nc, but al" fo im–
perfeét and irregul, r an admixtu re, as not to be e' pa–
ble of fa good apoli/h as the ehalecdony; and appear–
ing of a dufl¡y anu foul furfaee, tiU thrown imo water,
in ",hich they beeollle lucid, and in fome degrec tranf–
parent, either in p.\ft or
tot~Uy ;
alfo ehanging their
colour. wh ieh relurns lO themon being taken out of
the water.
To Ibis
~en\ls
belong the oeulus beli of authors, or
whitifh -grey hydroph,mes, variega1ed with y. Uuw, ¡nd
with 'a blaek central nucleus ; and the oeulus mundi,
or lapis muubilis, whieh is Iikewife a whilifh-grey kind
without veios.
HYDROPHOBIA, an
av~rfion
or drcad of water
j
a
H Y D
terrible {ymptom of the rabiel eaoina. See MEDICIMI,
HY
OIWPti
y
LLUM, In butany, a genu. of tbe pentaD–
dáa
mo~ogynia
claf,. The carolla
19
bell-fh.ped ; the
f1'gma IS bifid; and the eapfule is roundifh wilh t"'O
valves. Thcre are two fpecie" nooe of thero oalives
of Britaio.
HYDROPS, in medieioe, SeeMEDteINI.
HYDROSeOPE, an inllrument anciently ufed for !he
/lleafuring of time.
. The hydrofcope wal a kind of water·dock,
eonr.rl–Ing of a eylindrieal tub, conical at bonom : the eylin–
der was graduated, or marked OUt with divir.ons, tO
whieh the' top of the water becoming fuccellively con–
tiguo"s, as it tricJded out at the verte" of tbe CODe,
poioteu out tbe bour,
H Y D R O S T A
TIC
s.
T
HE
feieoeeof
H
YD~OSTA
TI
es treats of the oature
gravit y, prelfure, aod motioo of fluids in geDeral ;
.nd of weighiog folids in them.
A fluid is a body that yields to the leall prelfure or
difference of prelfures. !ts partid es are fa exeeedingly
fmall, that lhey eannot be difeerned by thebe(l of micro–
(,opes; lhey are hard, fi oee no fluid, exeepl air or Ileam,
can be prelfed ioto a lefs fpaee lhan il naluraUypolfelfes ;
and they are
roun~
and fmoolh,
fioe~
they are fa eafily
moved among one another.
AII bodies, bOlh fluid and folid, prefs downwards by
the force of gravity: but flu ids have this wonderful pro
perty, that their prelfure upwards and fidewife is equal
to their prelfure downwards; and lhis is always in pro.
portion to lheir perpendicular heighl, wilhout any re–
~ard
tO their quantilY: for, as eaeh partide is quile free
to move, it will move towards lhat pan or
r.deon
whieh lhe prelfure is leafl. And henee, no particle or
quaolily of a fluid can be al rell, till il is every way e-
4jually prtlred.
(Plate XCIX. fig. 2.) To fhew by experiment lhat
Iluids prefs up",ard as well as dowqward, let AB be a
long upright lube filled wilh IValer oear to ilS top ; and
CD a fmall tube 9pen at bOlh eods, and immerfed inlo
tbe waler in Ihe large one: if lhe immerfion be qUlCk,
yon will fce Ihe wate,r rife in the fmall tube to rhe
fa.meheighl that il (Iands In the great one, or Unltllhe lur
{aees of lhe water in bOlh are on the fame level : whieh
fhew! lhal the waler is
prelf~d
upward into lhe fmall tube
by the weigh'l of
Wh~l
is in the
grea~
ooe;
olherwi~e
it
cou!d never rife therem, conlrary lO lIS oatUr I eravuy ;
unlefs the
~iameter
of Ihe bore were fo fntall, Ihal lhe
amaétion of ¡he tube would raife the waler; whiell will
neva h.ppen, if the tube be as wide as Ihat in a eommon
haromeler. Ano as lhe waler rifes no Itigher in Ihe
fmall hlbe lhan lill ils furf,ee be on a lev(·1 ilh lhe fur
{ace of the waler in lhe great
one,
lhis fhews that lhe
r rclfure is nOl io proportion to.Ilte
qu~ntity
of IVa.ter in
the ¡:reat
lub~,
but
10
proporlton lO
liS
perpendlcul. r
heighl therein: for there is mleh more water in the
great tube all around the finall ooe, thao wnat is rai–
fed to lhe fame height in the {mall ooe, as it (Iaads in lhe
great.
Take out lhe
fma.lltube, and let ihe water rIIn OUI of
it; then it will be filled wilh airo Stop itl upper end
with lhe eork e, and it will be full of air all be/ow the
eork: this dooe, plunge it again to the bOllOmof the
water io Ihe great tube, aoJ you wiUfee the water rife
up io it
10
the height E ; whieh /hews lhat Ihe air is
¡
body, olherwife it eould not hinder lhe wm r
fromrir.ngup
10
Ihe fa me height as it did before, name/y,
t~
A;
and in fo
doi~g
il drove the air out at the tOP; but nOIf
the air is eonfioed by the eork e: aod it alfo fhe "'.
that lhe air is a eomprellible body; for if it were no!
fo, a drop of water could oot eoter inlo the tube.
'fhe prelfure of fluids being equal in all di reétions, it
rollows, that the fides of a velfel are as mlleh prelfed by
¡
fl uid in it, all around inany giveo ring of poi nls, as lhe
fl uid betow Ihat ring is prelfed by the weighl of al! Ihal
Ilands above il. Henee lhe prelfure upon every poinl in
lhe fides, immediately above lhe bOllom, is equal to the
prelfure upon every poiol of lh'e bOllom. To fhew this
by experimeot, let a hale be made at E (fig 3.) in the
fide of lhe lube AS cJofe by lhe boltom; and another
hole of the fame
r.zein lhe boltom, al C; then pour
water into lhe tube, keeping it fuI! as long asyou chufe
Ihe holes /hould run, and have tlVO tWO bafons ready
10
reeeive Ihe water lhat runs through Ihe two holes, until
you think there is enough in eaeh bafon; and you will
find , hy meafuring'the quainlilies. lh.l they He equ,l ;
whieh /hews that
th~
wmr ruo wilh equal freed throuch
bOl': holes: whieh it eould nOl have done, ir il
h~d
not
bl'en equally prelfrd throllgh Ihem both: for if • hole
of Ihe fame h ebe madein the
r.deof Ihe tube. as
,bOlIlI
f,
and if all lhree art permilled
10
rIln
togl·lh~r.
y"u .,11
fino that Ihe quanlily IIIn through lhe hole al
r i~ mll,~
Ids
Ihan ..hal has runin Ihe fame
tiUl~ lb(~lIgh
eilha of
lhe hules C or
l .
ID